Spacetime ❡
Das is alles von Gemini nur für mich zur Notiz
To see how different time values "stretch" or "shorten" the spacetime distance, we first have to solve a simple unit problem .
You cannot subtract seconds from meters . If you tried to calculate \text{meters}^2 - \text{seconds}^2, the math would break because the units don't match.
1. Where is the speed of light (c) used? ❡
To convert "time" into "meters" so they can live in the same equation, we multiply time (t) by the speed of light (c \approx 300,000,000 \text{ m/s}) :
\text{Time in meters} = c \times t
- If t is 2 seconds, then your time coordinate is:
c \times t = (300,000,000 \text{ m/s}) \times 2 \text{ s} = 600,000,000 \text{ meters}
- If t is 1 nanosecond, your time coordinate is:
(300,000,000 \text{ m/s}) \times 0.000000001 \text{ s} = 0.3 \text{ meters} (roughly 30 cm, the length of a ruler!)
In high-level physics (including your Doran & Lasenby book), we often define the speed of light as c = 1 . When we do this, "1 second" of time is literally treated as a distance: the distance light travels in one second (300,000\text{ km}) .
2. The 2-Meter Example (How time shifts the distance) ❡
Let's assume your 3D spatial distance is exactly d = 2\text{ meters} (so d^2 = 4).
Using the Spacetime Algebra (STA) signature from your book (e_t^2 = 1, e_i^2 = -1), the square of a spacetime vector X is :
\text{Interval}^2 = X^2 = (ct)^2 - d^2
X^2 = (ct)^2 - 4
Let’s look at how the "distance" squared (X^2) changes depending on how much time passes (ct):
Case A: ct is small (e.g., ct = 1\text{ meter}) ❡
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You only have enough time for light to travel 1\text{ meter}, but you need to cover 2\text{ meters} of space.
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Math: X^2 = 1^2 - 4 = -3
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Meaning: The interval squared is negative . In relativity, this is called a spacelike interval . It means space dominates. It is physically impossible for any signal to connect these two points, because they are too far apart in space and too close in time .
Case B: ct is exactly 2\text{ meters} ❡
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You have exactly enough time for light to travel the 2\text{ meters} of space.
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Math: X^2 = 2^2 - 4 = 0
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Meaning: The spacetime distance is exactly zero ! This is a lightlike (or null) interval . A photon of light emitted at the start of your trajectory will reach the end. From the photon's perspective, zero time and zero distance have passed .
Case C: ct is large (e.g., ct = 5\text{ meters}) ❡
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You have plenty of time (enough for light to travel 5\text{ meters}) to cross just 2\text{ meters} of space.
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Math: X^2 = 5^2 - 4 = 21
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Meaning: The interval squared is positive . This is a timelike interval . Time dominates. You (a massive observer) can easily travel between these two points because you can move slower than the speed of light and still make it in time .
By using +1 for the time dimension and -1 for the spatial dimensions, the math naturally groups your 4D coordinates into these three physical categories (Spacelike, Lightlike, Timelike) based on whether the result of the squaring is negative, zero, or positive !